<p>In this paper, we consider the following fractional Hamiltonian system, <Equation ID="Equ51"> <EquationSource Format="TEX">\(\begin{aligned} \begin{aligned} {\left\{ \begin{array}{ll} (-\Delta )^{s}u = g(x,v) &amp; \text{ in } \Omega ,\\ (-\Delta )^{s}v = f(x,u) &amp; \text{ in } \Omega ,\\ u\ge 0, v\ge 0 \quad &amp; \text{ in } \Omega ,\\ u=v=0 \quad &amp; \text{ in } {\mathbb {R}}^{N}\setminus \Omega , \end{array}\right. } \end{aligned} \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">)</mo> </mrow> <mi>s</mi> </msup> <mi>u</mi> <mo>=</mo> <mi>g</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>v</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">)</mo> </mrow> <mi>s</mi> </msup> <mi>v</mi> <mo>=</mo> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mi>u</mi> <mo>≥</mo> <mn>0</mn> <mo>,</mo> <mi>v</mi> <mo>≥</mo> <mn>0</mn> <mspace width="1em" /> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mi>u</mi> <mo>=</mo> <mi>v</mi> <mo>=</mo> <mn>0</mn> <mspace width="1em" /> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo lspace="0.15em" rspace="0.15em" stretchy="false">\</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(s\in (0,1),\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(N&gt;2s,\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>&gt;</mo> <mn>2</mn> <mi>s</mi> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\Omega \subset {\mathbb {R}}^N\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ω</mi> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> is a smooth bounded domain and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(f,g:\overline{\Omega } \times {\mathbb {R}} \rightarrow {\mathbb {R}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>f</mi> <mo>,</mo> <mi>g</mi> <mo>:</mo> <mover accent="true"> <mi mathvariant="normal">Ω</mi> <mo>¯</mo> </mover> <mo>×</mo> <mi mathvariant="double-struck">R</mi> <mo stretchy="false">→</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation> are continuous functions. By variational method and fractional Orlicz-Sobolev spaces, we demonstrate the existence of nontrivial weak solutions. As far as we know, there are few research works devoted to the fractional Hamiltonian system on a bounded domain. Our work exhibits threefold of novelties. Firstly, we deal with a non-autonomous system; the upper bound restriction required in previous works is no longer needed; moreover, we can treat almost critical nonlinearities (see (<InternalRef RefID="Equ18">1.18</InternalRef>) below).</p>

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Existence of solutions for a nonlocal elliptic system in fractional Orlicz-Sobolev spaces

  • Jia Zhang

摘要

In this paper, we consider the following fractional Hamiltonian system, \(\begin{aligned} \begin{aligned} {\left\{ \begin{array}{ll} (-\Delta )^{s}u = g(x,v) & \text{ in } \Omega ,\\ (-\Delta )^{s}v = f(x,u) & \text{ in } \Omega ,\\ u\ge 0, v\ge 0 \quad & \text{ in } \Omega ,\\ u=v=0 \quad & \text{ in } {\mathbb {R}}^{N}\setminus \Omega , \end{array}\right. } \end{aligned} \end{aligned}\) ( - Δ ) s u = g ( x , v ) in Ω , ( - Δ ) s v = f ( x , u ) in Ω , u 0 , v 0 in Ω , u = v = 0 in R N \ Ω , where \(s\in (0,1),\) s ( 0 , 1 ) , \(N>2s,\) N > 2 s , \(\Omega \subset {\mathbb {R}}^N\) Ω R N is a smooth bounded domain and \(f,g:\overline{\Omega } \times {\mathbb {R}} \rightarrow {\mathbb {R}}\) f , g : Ω ¯ × R R are continuous functions. By variational method and fractional Orlicz-Sobolev spaces, we demonstrate the existence of nontrivial weak solutions. As far as we know, there are few research works devoted to the fractional Hamiltonian system on a bounded domain. Our work exhibits threefold of novelties. Firstly, we deal with a non-autonomous system; the upper bound restriction required in previous works is no longer needed; moreover, we can treat almost critical nonlinearities (see (1.18) below).